First determination of the $${\rho }$$ ρ parameter at $${\sqrt{s} = 13}$$ s=13 TeV: probing the existence of a colourless C-odd three-gluon compound state

Abstract

Abstract The TOTEM experiment at the LHC has performed the first measurement at $$\sqrt{s} = 13\,\mathrm{TeV}$$ s=13TeV of the $$\rho $$ ρ parameter, the real to imaginary ratio of the nuclear elastic scattering amplitude at $$t=0$$ t=0 , obtaining the following results: $$\rho = 0.09 \pm 0.01$$ ρ=0.09±0.01 and $$\rho = 0.10 \pm 0.01$$ ρ=0.10±0.01 , depending on different physics assumptions and mathematical modelling. The unprecedented precision of the $$\rho $$ ρ measurement, combined with the TOTEM total cross-section measurements in an energy range larger than $$10\,\mathrm{TeV}$$ 10TeV (from 2.76 to $$13\,\mathrm{TeV}$$ 13TeV ), has implied the exclusion of all the models classified and published by COMPETE. The $$\rho $$ ρ results obtained by TOTEM are compatible with the predictions, from other theoretical models both in the Regge-like framework and in the QCD framework, of a crossing-odd colourless 3-gluon compound state exchange in the t-channel of the proton–proton elastic scattering. On the contrary, if shown that the crossing-odd 3-gluon compound state t-channel exchange is not of importance for the description of elastic scattering, the $$\rho $$ ρ value determined by TOTEM would represent a first evidence of a slowing down of the total cross-section growth at higher energies. The very low-|t| reach allowed also to determine the absolute normalisation using the Coulomb amplitude for the first time at the LHC and obtain a new total proton–proton cross-section measurement $$\sigma _{\mathrm{tot}} = (110.3 \pm 3.5)\,\mathrm{mb}$$ σtot=(110.3±3.5)mb , completely independent from the previous TOTEM determination. Combining the two TOTEM results yields $$\sigma _{\mathrm{tot}} = (110.5 \pm 2.4)\,\mathrm{mb}$$ σtot=(110.5±2.4)mb .